Table 6.
Case | Figures | Modes | ree (mm) | G es | G se | a 1 − 1 | a 10 | a 11 |
---|---|---|---|---|---|---|---|---|
All | 5–8 | 00 | * | 0.77 | 7.77 | — | — | — |
Default | 5B | 1-1 | 60 | 0.77 | 7.77 | 1 | 0 | 0 |
Small Splitting | 5D, E | 1-1 | 50 | 0.82 | 9.8 | 1 | 0 | 0 |
Large Splitting | 5F, G | 1-1 | 70 | 0.98 | 11.3 | 1 | 0 | 0 |
Increased Gain | 5B, C | 1-1 | 60 | 0.88 | 10.5 | 1 | 0 | 0 |
Single Alpha | 6 | 1-1 | 50 | 0.82 | 9.8 | − 0.08 | 0 | 0 |
Double Alpha | 7 | 1-1,11 | 70 | 0.98 | 11.3 | 0.69 | 0 | 1.10 |
Mu | 8B–D | 10 | 50 | 0.82 | 9.8 | 0 | − 0.09 | 0 |
Tau | 8F–H | 11 | 50 | 0.82 | 9.8 | 0 | 0 | 0.32 |
The 00 mode has the parameters listed in the row labeled All in every case, except that the asterisk indicates that the same value of ree is to be used as for the other modes in each case listed in subsequent rows. In other instances, the listed l = 1 modes have the parameters given. Parameters not shown are as in Table 1 and modes not listed are omitted from the case in question.